Method and apparatus for generation and amplification of light in a semi-guiding high aspect ratio core fiber
Abstract
A planar laser gain medium and laser system. The novel laser gain medium includes an active core having a high aspect ratio cross-section with a fast-axis dimension and a slow-axis dimension, signal claddings adapted to form reflective boundaries at fast-axis boundaries of the core, and a material adapted to minimize reflections at slow-axis boundaries of the core. In an illustrative embodiment, the laser gain medium is an optical fiber. The core and claddings form a waveguide adapted to control modes propagating in the fast-axis direction. When the laser gain medium is employed as a laser oscillator, a high reflectivity mirror and an outcoupler are positioned at opposite ends of the core to form a laser resonator adapted to control modes in the slow-axis direction.
Claims
exact text as granted — not AI-modified1 . A laser system comprising:
a laser gain medium having an active core with a high aspect ratio cross-section; pumping means for exciting said laser gain medium to generate laser energy; waveguiding means for mode control of said laser energy along a fast-axis direction of said core; and resonator means for mode control of said laser energy along a slow-axis direction of said core.
2 . The system of claim 1 wherein said laser gain medium is an optical fiber.
3 . The system of claim 1 wherein said waveguiding means includes signal claddings disposed in contact with fast-axis boundaries of said core.
4 . The system of claim 3 wherein said signal claddings have a refractive index less than a refractive index of said core such that light in said core is trapped by total internal reflection in said fast-axis direction.
5 . The system of claim 4 wherein said refractive index of said signal claddings is reduced relative to that of said core by modifying dopant concentrations in said claddings.
6 . The system of claim 4 wherein said refractive index of said signal claddings is reduced relative to that of said core by including a micro-structure in said claddings.
7 . The system of claim 3 wherein said claddings include a micro-structure adapted to trap light in said core according to principles of photonic bandgaps.
8 . The system of claim 1 wherein a thickness of said core is matched to a numerical aperture of said core such that said core is a single-mode planar waveguide in said fast-axis direction.
9 . The system of claim 1 wherein a thickness of said core is adapted to support multiple modes in said fast-axis direction.
10 . The system of claim 9 wherein said system further includes means for stripping-out higher-order modes from said core.
11 . The system of claim 10 wherein said system includes means for coiling said laser gain medium with a coil radius adapted to present a high loss to higher-order modes but a low loss to a lowest-order mode.
12 . The system of claim 1 wherein said active core is optically open in said slow-axis direction.
13 . The system of claim 1 wherein width and gain value of said active core and length of said laser gain medium are specified in such a manner to enable gain guiding in a slow-axis direction.
14 . The system of claim 1 wherein said resonator means includes a mirror and an outcoupler positioned at opposite ends of said core to form a laser resonator.
15 . The system of claim 14 wherein sizes, curvatures, and spacing of said mirror and outcoupler are chosen to control modes propagating in said core in said slow-axis direction.
16 . The system of claim 14 wherein said mirror and outcoupler form a stable resonator.
17 . The system of claim 16 wherein a size of said outcoupler is chosen to produce a planar resonator Fresnel number less than unity.
18 . The system of claim 16 wherein a length of said resonator is chosen such that a lowest-order mode overfills said core such that its average size exceeds approximately twice the width of said core.
19 . The system of claim 18 wherein a size of said outcoupler is chosen such that said average mode size exceeds said outcoupler size by approximately a factor of two.
20 . The system of claim 14 wherein said mirror and outcoupler form a short unstable resonator.
21 . The system of claim 1 wherein said system further includes means for applying local and/or distributed twists of said laser gain medium to create and control an effective planar lens.
22 . The system of claim 2 wherein said resonator means are integrated into said fiber.
23 . The system of claim 2 wherein said system further includes an end-cap fused to an end of said fiber for expanding an output laser beam.
24 . The system of claim 23 wherein said end-cap has an exit surface that is shaped to control a divergence of said output beam.
25 . The system of claim 23 wherein said end-cap has an exit surface that is shaped to collimate said output beam.
26 . A laser system comprising:
an optical fiber having an active core with a high aspect ratio cross section, and signal claddings positioned in contact with said core and adapted to control modes along a fast-axis direction of said core; one or more pump apparatuses for coupling pump energy into said core to generate laser energy; and a mirror and an outcoupler positioned at opposite ends of said fiber core to form a laser resonator adapted to control modes of said laser energy along a slow-axis of said core.
27 . The system of claim 26 wherein said active core is optically open in said slow-axis direction.
28 . The system of claim 26 wherein width and gain value of said active core and the length of said optical fiber are specified in such a manner to enable gain guiding in a slow-axis direction.
29 . The system of claim 26 wherein said mirror and outcoupler are integrated into said fiber.
30 . The system of claim 26 wherein said fiber further includes a glass foil surrounding said core and signal claddings.
31 . The system of claim 26 wherein said system further includes a mechanism for applying local and/or distributed twists of the fiber to create and control an effective planar lens in said laser resonator.
32 . The system of claim 26 wherein each pump apparatus is adapted to focus a pump beam at a slanted angle into said fiber.
33 . The system of claim 26 wherein said pump apparatuses are positioned near edges of said fiber beyond said core.
34 . The system of claim 26 wherein said pump apparatuses are oriented facing toward said mirror.
35 . The system of claim 26 wherein said pump apparatuses are concentrated closer to said outcoupler than said mirror.
36 . The system of claim 26 wherein said pump apparatuses include optical prisms placed in optical contact with said fiber.
37 . The system of claim 26 wherein said pump apparatuses include fiber pigtails adapted to couple pump light into edges of said fiber.
38 . The system of claim 37 wherein said fiber pigtails are integrated into said fiber.
39 . The system of claim 38 wherein said fiber pigtails have high aspect ratio cores.
40 . The system of claim 26 wherein said system further includes an end-cap attached to an outcoupler end of said fiber for expanding an output laser beam.
41 . The system of claim 40 wherein said end-cap has an exit surface that is shaped to control a divergence of said output beam.
42 . The system of claim 40 wherein said end-cap has an exit surface that is shaped to collimate said output beam.
43 . An optical arrangement comprising:
a plurality of planar core fibers arranged sequentially end to end, each fiber having a slow axis oriented orthogonal to slow axes of neighboring fibers and focusing optics adapted to transform a near-field profile from an output of one fiber to a far-field profile at an input of a subsequent next fiber.
44 . The arrangement of claim 43 wherein each fiber includes a high-aspect ratio cross-section core, and claddings positioned in contact with said core to control modes along a fast axis of said core
45 . The arrangement of claim 43 wherein each fiber is optically open along a slow axis of said core.
46 . The arrangement of claim 43 wherein said focusing optics include a positive lens disposed between ends of two neighboring fibers.
47 . The arrangement of claim 46 wherein ends of neighboring fibers are spaced at a distance equal to twice a focal length of said lens.
48 . The arrangement of claim 43 wherein said focusing optics include a glass gradient index lens disposed between ends of two neighboring fibers.
49 . The arrangement of claim 48 wherein ends of neighboring fibers are spaced at a distance equal to a focal length of said lens.
50 . The arrangement of claim 43 wherein said arrangement further includes a mechanism for applying local and/or distributed twists of said fibers to create and control an effective planar lens.
51 . The arrangement of claim 43 wherein said arrangement further includes one or more end-caps attached to ends of said fibers for expanding a signal beam.
52 . The arrangement of the claim 43 wherein said fibers include one or more additional components that are integrated into said fibers.
53 . The arrangement of claim 43 wherein said arrangement forms a laser amplifier.
54 . The arrangement of claim 43 wherein said arrangement further includes a mirror and an outcoupler positioned at opposite ends of said arrangement to form a laser resonator.
55 . A laser system comprising:
an optical fiber having an active core with a high aspect ratio cross section, and signal claddings positioned in contact with said core and adapted to control modes along a fast-axis direction of said core; and a material disposed in contact with said core at narrow edges of said core and adapted to minimize reflections in a slow-axis direction of said core; and a plurality of on-ramp fiber pigtails integrated into said fiber for coupling pump energy into said active core to generate laser energy.
56 . The system of claim 55 wherein said core is optically open in said slow-axis direction.
57 . The system of claim 55 wherein a material disposed has a refractive index that provides anti-guiding along a slow-axis direction.
58 . The system of claim 55 wherein width and gain value of said active core and length of said optical fiber are specified in such a manner to enable gain guiding in a slow-axis direction.
59 . The system of claim 55 wherein said fiber pigtails have high aspect ratio cores.
60 . The system of claim 55 wherein said fiber pigtails have rectangular cores.
61 . The system of claim 55 wherein said fiber pigtails have cores shaped to match a beam shape of said pump energy.
62 . The system of claim 55 wherein said fiber pigtails are adapted to couple pump energy at a slanted angle into said fiber.
63 . The system of claim 55 wherein said fiber pigtails are adapted to couple pump energy into edges of said fiber.
64 . The system of claim 55 wherein said system further includes a mirror and an outcoupler positioned at opposite ends of said fiber core to form a laser resonator adapted to control modes along a slow-axis of said core.
65 . The system of claim 64 wherein said fiber pigtails are oriented facing toward said mirror.
66 . The system of claim 64 wherein said fiber pigtails are concentrated closer to said outcoupler than said mirror.
67 . The system of claim 64 wherein said mirror and outcoupler are integrated into said fiber.
68 . The system of claim 55 wherein said system further includes an end-cap attached to an outcoupler end of said fiber for expanding an output laser beam.
69 . The system of claim 68 wherein said end-cap has an exit surface that is shaped to control a divergence of said output beam.
70 . The system of claim 68 wherein said end-cap has an exit surface that is shaped to collimate said output beam.
71 . A device for coupling pump energy into a planar fiber comprising:
a glass prism placed in optical contact with a surface of said planar fiber and one or more fiber pigtails fused within said glass prism at a large angle to a prism surface and having an end in contact with said surface of said planar fiber.
72 . The device of claim 71 wherein a numerical aperture of a core of said fiber pigtail is no more than half of a numerical aperture of a pump guiding channel in said planar fiber.
73 . The device of claim 71 wherein a tilt angle of said fiber pigtail inside said prism is close to a numerical aperture of a core of said fiber pigtail.
74 . The device of claim 71 wherein a face of said prism in contact with said planar fiber beyond a core footprint of said fiber pigtail is partially coated with a high reflectivity coating.
75 . A method for generating laser energy, the method comprising:
arranging a plurality of planar core fibers sequentially end to end, with each fiber having a slow axis oriented orthogonal to slow axes of neighboring fibers; and transforming a near-field profile from an output of one fiber to a far-field profile at an input of a subsequent next fiber.
76 . A method for coupling pump energy into an optical fiber, the method comprising:
integrating a plurality of on-ramp fiber pigtails into said fiber; coupling pump energy from a pump source to said fiber through said pigtails; and matching cores within said pigtails to a beam shape of said pump energy.Join the waitlist — get patent alerts
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